Alphabeta Math
DefinitionDefinition: Literature-sourcedProof: Not applicablePipeline-generatedjudge pass (gpt-6.1-sol)
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Deformation to the normal cone and specialization

Definition

Assume the Axiom of Choice (The Axiom of Choice) inherited from the smooth normal-sequence suppliers. For a closed immersion i:X↪Y with ideal I, put CXY=Spec⁡X(⨁n≥0In/In+1) and M=Bl⁡X×{∞}(Y×P1). Let B=Bl⁡XY be the strict transform of Y×{∞}. The fibre at infinity is the sum M∞=B+P(CXY⊕1) of effective Cartier divisors, whose intersection is P(CXY); this is a union with a common boundary, not a disjoint union. Projectivized cones here use the lines convention Proj⁡(gr⁡IOY[S]). Off infinity M≅Y×A1, and Di:=M∖B has special fibre CXY and ordinary fibres Y. It is flat over P1. The specialization σi:Am(Y)→Am(CXY) is obtained by extending the flat pullback of a cycle to Di, then taking Cartier Gysin at infinity. It sends an integral [V] to the fundamental cycle [CX∩VV] pushed to CXY. For a regular immersion of codimension d, the normal cone equals the rank-d normal bundle NX/Y. The construction works for finite type schemes over a field, with locally finite cycles in the locally finite type case.

Well-definedness. The charts of M near infinity are computed directly: over an affine open Spec⁡A⊆Y with X=Spec⁡(A/I) and t the coordinate vanishing at infinity, the t-chart of the blowup is the affine blowup algebra A[t,I/t]=∑n≥0t−nIn[t]⊆A[t,t−1], and multiplication by t is injective with quotient gr⁡IA; in the chart of a generator a∈I the ring is A[I/a][t/a], and t=a(t/a) exhibits the fibre at t=0 as the sum of the exceptional divisor a=0 and the strict transform t/a=0, whose charts are Bl⁡XY and whose intersection is Proj⁡gr⁡IA. This identifies the fibre at infinity as the stated union of effective Cartier divisors, without assuming Y integral or the centre Cartier, and shows that, away from infinity, M∖B≅Y×A1, while its special fibre is CXY; the charts are torsion-free over k[t] (or polynomial over the affine blowup algebras), and a torsion-free module over the principal ideal domain k[t] is flat, giving flatness of M over P1 (compare the chart computation of Smooth immersions, their conormal sequence, deformation charts and smooth sections). Localization for the pair CXY↪M∖B gives a lift of the pulled-back cycle class to Di, and two lifts differ by a class supported on CXY; the Cartier Gysin at infinity kills that difference because the normal line of the infinity fibre is trivial, so j!j∗γ=c1(O)∩γ=0 by the basic property c1(OX)=0 of Intersection with an invertible sheaf and the first Chern class; hence σi is well defined on Chow classes. On an integral cycle [V] the closure of V×A1 in the t-chart is Spec⁡OV[t,IOV/t], and cutting by t produces gr⁡IOVOV, which is the fundamental cycle of the normal cone CX∩VV with its generic lengths; for a regular sequence generating I, Associated graded algebra of an ideal generated by a regular sequence identifies gr⁡IA with Sym⁡A/I(I/I2), so the cone is the rank-d normal bundle of Smooth immersions, their conormal sequence, deformation charts and smooth sections.

Depends on

Used by

Dependency tree · two levels

55 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.

Sources